Construction and Building Materials 189 (2018) 816–824 Contents lists available at ScienceDirect Construction and Building Materials journal homepage: www.elsevier.com/locate/conbuildmat Numerical modeling for crack self-healing concrete by microbial calcium carbonate Hassan Amer Algaifi a,⇑, Suhaimi Abu Bakar a, Abdul Rahman Mohd. Sam b, Ahmad Razin Zainal Abidin a, Shafinaz Shahir c, Wahid Ali Hamood AL-Towayti c a Department of Structure and Materials, School of Civil Engineering, Faculty of Engineering, Universiti Teknologi Malaysia, Johor, Malaysia UTM Construction Research Centre, Institute for Smart Infrastructure and Innovative Construction, School of Civil Engineering, Faculty of Engineering, Universiti Teknologi Malaysia, Johor, Malaysia c Department of Biosciences, Faculty of Science, Universiti Teknologi Malaysia, Johor, Malaysia b h i g h l i g h t s The developed model is able to predict the bioconcrete crack-healing relatively well. A crack width of 0.4 mm was healed at 70 days compared to 60 days in the model. With the increasing of urea hydrolysis, more calcium carbonate could be formed. The hydrolysis of urea induces the diffusive transport mechanism to the boundary. a r t i c l e i n f o Article history: Received 3 March 2018 Received in revised form 30 August 2018 Accepted 31 August 2018 Available online 18 September 2018 Keywords: Crack-healing concrete Crack-healing modeling Bacteria-based healing a b s t r a c t The inevitable existence of microcracks in concrete matrix can create interconnected flow paths due to external load, which will then provide easy access to harmful substances, and thus yielding to corrosion of reinforcement. Consequently, this affects the durability of the structure. Recent researches are devoted in crack self-healing concrete, which mimics the natural remarkable biological system of wounds healing. Despite that, the issue revolving around the efficiency of crack self-healing technique remains important. Microbial calcium carbonate offers an attractive biotechnique to fill pores volume as well as both micro and macrocracks in the affected cementitious material, resulting in barriers to inhibit water or aggressive chemical flow. However, results of this approach have only been demonstrated at laboratory scale and theoretical information is still limited. The present study describes a theoretical model to simulate the kinetics of calcite precipitation induced in response to the hydrolysis of urea in concrete crack. In addition, a second-order partial differential equation in time and space to model the healing process, rationally based on physic-bio-chemical issues, was developed. Both finite element and finite difference were implemented to solve this equation. SEM images were conducted to verify the predicted crack-healing results through artificial cracked mortar specimens incorporating indigenous Lysinibacillus sphaericus. As such, it could be concluded that a prediction of the healing process of the affected cementitious materials can be provided via the developed model. Ó 2018 Elsevier Ltd. All rights reserved. 1. Introduction Inevitable microcracks remain to be a challenge to civil engineers as they are considered as a threat to the durability of structures. Such microcracks, porosity and interconnectivity of pores volume create an easy pathway for harmful substances to enter and cause reinforcement corrosion [1–6]. However, concrete is ⇑ Corresponding author. E-mail address: [email protected] (H.A. Algaifi). https://doi.org/10.1016/j.conbuildmat.2018.08.218 0950-0618/Ó 2018 Elsevier Ltd. All rights reserved. capable of plugging these microcracks themselves, which is well known as autogenous healing. Nonetheless, the ability is still limited to crack width that is less than 0.06 mm [7]. Various manual cracks repairing techniques are available to extend the life of structures. However, several drawbacks have been detected such as short period of time (10–15 years), high cost, difficult-to-access locations and the fact that most traditional repair techniques are polymer based that lead to hazards associated with the environment and health [8]. H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 Therefore, researchers have devoted considerable efforts to mimic natural biohealing by incorporating bacteria in cementitious material in recent years. The direct use of bacteria with their nutrients in fresh concrete mix without human intervention was first proposed by Jonkers and colleagues [9–12]. The potential ability of bacteria to seal cracks through the formation of calcium carbonate was investigated through different mechanisms such as sulfate reduction bacteria [13,14], oxidation of organic acids [15– 17], nitrate reduction bacteria [18,19] and ureolytic bacteria [20,21]. 0.46 mm of concrete crack-width was completely healed after 100 days via Bacillus alkalinitrilicus, while ureolytic bacterial has proven its ability to heal crack widths of up to 0.97 mm in 8 weeks of water submission [22,23]. In the same context, nitrate reducing bacteria also showed its capability to heal crack widths of 0.46 mm in 56 days [18]. However, most of these studies have only focused primarily on both laboratory and experimental work and they are still suffering from the lack of numerical simulation to accurately predict experimental behaviour, which can result in the decrease of cost. Examples of mathematics researches of polymer self-healing are available in the previous studies [24–30]. On the other hand, computational research into self-healing concrete is still in its infancy stage and there are only a few numerical modelling involving the healing process of affected cementitious material. Autogenous crack-healing in cementitious material through further hydration was mathematically simulated using water transport theory, ion diffusion model and thermodynamics model [31]. The results showed that the rate of healing processing speed increased according to the amount of water available that was assumed to be in a capsule. Further modelling study was focused on the interaction between the crack and embedded micro-capsule in cementitious material [32]. In addition, autogenous self-healing concrete by calcium carbonate due to the carbonation of dissolved calcium hydroxide was also developed byAlikoBenítez, Doblaré [33]. Moving from Autogenous self-healing model to bacteria-based self-healing, a numerical model was developed to describe the healing process of cracks in concrete using bacteria, which relies on the oxidation of organic acids [34]. The diffusion of the healing agent over the crack is governed by diffusion equation which is solved using Galerkin finite element, while the evolution of moving boundary due to calcite precipitation is solved using level set method. In this study, indigenous ureolytic bacteria was utilised to induce microbial calcium carbonate by releasing urease enzyme, which in turn stimulated the urea degradation to carbonate and ammonium under appropriate condition as expressed in Eq. (1) [35]. At the same time, the formation of calcite would develop due to the reaction between the carbonate and calcium ions on the cell wall of the bacteria since it is negatively charged, which was specifically considered as bacterial aggregate as shown in Eq. (2). urease 817 COðNH2 Þ2 þ 2H2 O ! 2NHþ4 þ CO2 3 ð1Þ Ca þ CO2 3 ! CaCO3 ð2Þ The evolution of bacterial aggregate was predicted by developing a numerical model. In the said model, urea, calcium, nutrient and bacteria were pre-mixed in the concrete matrix and distributed homogeneously. In addition, urea was assumed to be stored in capsules, which would break if they were intersected by a crack. On the contrary, bacteria, nutrient and calcium were assumed to exist in the crack domain. Consequently, with water and nutrients, the spores of the bacteria would germinate and reproduce, and thus limestone would develop in the crack as shown in Fig. 1. In other words, both the urea and calcium (artificial blood platelet) would be recruited to the damage area to block the water filled crack. This mechanism was inspired by the idea of blood clotting in skin wounds via platelet, which exists in the blood, and ultimately, stops the bleeding. Specifically, the said process was mathematically simulated using a system of equations including first-order ordinary differential equation and second order partial differential equation, in which both finite difference and finite element methods were used to solve the said form of bio-chemical-diffusive model. 2. Mathematical development of the model 2.1. Model description In this study, the model is schematically shown in Fig. 2. A macro-crack with the size of 20 mm (length) 0.4 mm (width) 20 mm (depth) was supposed to pass through a capsule. In addition, the crack domain was also assumed to be filled with water instantaneously. The model was developed rationally, relying on the physics, biology and chemistry of the healing process respectively. Firstly, urea was recruited to the damage area due to the flux (F). In our model, flux denoted that the ion species are allowed to diffuse as a consequence of a natural movement from a high concentration area to a low concentration area inside the cracks developed in the concrete cover. The mechanism of diffusive was governed by Fick’s first law for ion species as shown in Eq. (3), where c is the concentration of species in mol/m3, D is the diffusion coefficient in unit of m2/day and flux F is in units of mol/m2 day. F ¼ D @c @x ð3Þ Secondly, calcium ions would stick and gather on the bacteria cells that release urease enzyme to catalyse the decomposition of urea to carbonate ions. These bacteria cells exist in all boundaries of the crack with different numbers since cell growth cannot repro- Fig. 1. The evolution of a crack closing in different stages. 818 H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 Fig. 2. Schematic diagram of evolving bacteria aggregate. duce in the absence of oxygen such as in the deeper parts of the cracks. In other words, if higher bacterial cells concentration (a) is achieved, more urea hydrolysis can be formed, which was taken into account in the proposed model [36]. The initial cell concentration was taken as 105 cell/cm3 at deeper part of the crack according to Zemskov, Jonkers [34],while the bacterial cells were considered as the optimum cell concentration 108 cell/cm3 at the crack mouth (cracks surface). According to mass action law and stoichiometry, urea hydrolysis can be formalised mathematically. Dynamical system was utilised to model the concentration of urea species over time using ordinary differential equation and a first order rate reaction was proposed as shown in Eq. (4). It should be mentioned that the urea species COðNH2 Þ2 and calcite species ½CaCO3 (concentration is denoted by brackets) are treated as dynamic species which consume and accumulate with time, respectively. @ CO ðNH2 Þ2 @c ¼ ¼ k1 a c @t @t ureolysis ureolysis concentration at each node and 1 day Thirdly, the formation of calcium carbonate would start to precipitate according to Eq. (2), which states that the microbial calcium carbonate is the product of the chemical reaction between calcium and carbonate ions. This carbonate ion is in equimolar with urea hydrolysis according to Eq. (1). In the proposed model, the evolution of urea hydrolysis was the main sole parameter to affect the productivity of calcite since sufficient amount of calcium was assumed to be available in the damaged area, similar to bacterial nutrient. Therefore, the evolution of calcite with time was taken into account as pseudo first-order reaction and is as expressed in Eq. (5), according to mass balance and stoichiometry. h i @ ½CaCO3 @c ¼ þk2 CO2 ¼ þk 2 3 @t @t ureolysis which k2 ¼ calcium carbonate precipitation rate ð5Þ M ðCaCO3 Þ:h qCaCO3 Eq. (3) is analogous to the one-dimensional stress/strain law for the stress analysis problem which is rx ¼ E @u . The minus sign @x indicates that the species flow from regions of higher concentration to regions of lower concentration. Moreover, it states that the flux in the x direction is proportional to the gradient of concentration in the x direction. Similarly, the concentration gradient at x þ dx is evaluated F xþdx ¼ D 1 day ð6Þ The calculations were automatically stopped if the healing ratio was S ¼ VVh 1. As such, if S = 1, the volume of the crack could be said @c @xxþdx ð7Þ In the present model, the diffusion flux and concentration gradient of species at a particular point in a crack domain varied with time, with a net depletion of the diffusing species that can be depicted by a control volume as shown in Fig. 3. This could be expressed mathematically as shown in Eq. (8). Flux in = Flux out + accumulation rate + consumption (losses by bacteria) F x F xþdx ¼ @ci @ci dx þ dx @t @t depletion ð8Þ Eq. (8) denotes that the flux in of the species urea minus the flux out is equal to the amount of accumulation rate into this volume element plus the depletion of species due to the reaction. This is discussed in detail in the following section. Using a two-term of Taylor series to expand the flux out F xþdx , the equation could be expressed as: @c @t ) Once the calcite concentration was calculated, the volume of calcite precipitates (healed volume) inside the crack domain is as expressed in Eq. (6), whereV is the volume of crack, V h is the crack healed volume, qCaCO3 ¼ 2:711 cmg 3 ; the molar mass of calcite is g M ðCaCO3 Þ ¼ 100:0869 mole and h is the amount of calcite precipitation (mole). V h ¼ V CaCO3 ¼ 2.2. hydrolysis-diffusion equation ð4Þ In which a ¼ aami , am is optimum cells concentration, ai is cells k1 ¼ ureolysis rate constant to have been filled with calcite, which would result in maximum healing capacity. On the contrary, the healing product has yet to start precipitate if S = 0. 2 @ c ¼ D @x 2 @c @t @c @t ureolysis @ c ¼ D @x 2 k1 a c 2 ð9Þ Once the boundary and initial conditions were prescribed for the species, the model was then completely defined through one ordinary differential Eq. (5) and a second-order partial differential Eq. (9). 2.3. Numerical implementation Eq. (9) represents the consumption –diffusion differential equation, which can be solved using the finite element method by dividing the problem domain into finite length, one dimensional element and discretising the distribution of urea concentration within each element as shown in the following equation. cðx; t Þ ¼¼ N1 ðxÞc1 ðtÞ þ N2 ðxÞc2 ðtÞ ð10Þ 819 H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 Fig. 3. Control volume for one dimensional diffusion with depletion. where a two-node linear element (shape function Ni ) were used similar to the displacement function of truss equation as shown below: 3. Verification of the predicted Crack-Healing results x N1 ðxÞ ¼ 1 ; L For the purpose of verification of the predicted crack healing results, experimental work was carried out to support the proposed model. Accordingly, indigenous Lysinibacillus sphaericus was isolated from 10 cm of the ground surface located in Universiti Teknologi Malaysia (1°330 52.400 N 103°390 16.300 E). It was tested for its capability to survive in a harsh environment, such as concrete and induce calcium carbonate, in response to hydrolysis of urea. It demonstrated a positive result, which was consistent with previous studies[37,38]. Subsequently, the partial sequencing of the bacterial genetic code 16S rRNA was deposited in the gene bank database under the accession number of MG928532. In addition, it was stored as glycerol stock at 80 °C for future use[17]. N 2 ð xÞ ¼ x L By applying Galerkin’s finite element method to Eq. (9), the following is obtained: Z L N i ð xÞ 0 ! @c @2c D 2 þ k1 ac Adx ¼ 0 @t @x i ¼ 1; 2 ð11Þ Subsequently, using the integration by parts to the second term and integration to the first and third terms of Eq. (11), it becomes: LA 2 1 6 1 2 c_ 1 c_ 2 þ AD 1 1 L 1 1 c1 c2 þ Aak1 L 2 1 c1 ¼ 6 1 2 c2 F1 F2 ð12Þ For simplicity, Eq. (12) could be expressed as: ½mfc_ g þ ½kfcg þ kg fcg ¼ ff g ð13Þ Eq. (13) represents a first-order differential equations in time. Element nodes were assigned to the global nodes and the element matrix was added to the appropriate global matrix, and thus yielding the global equation as the following. n o ½M C_ þ ½K fC g þ K g fC g ¼ fF g ð14Þ The forward finite difference method was used as a simple approach to obtain the solution to both Eqs. (5) and (14). To apply the concept of Euler’s method, which is known as a forward finite difference, the time derivative approximation of the nodal concentration matrix took place as: fC iþ1 g fC i g C_ ffi Dt ð15Þ ½M fC i gg þ ½K fC g þ K g fC g ¼ fF 0 g ) fC iþ1 g ¼ fC i g þ Dt½M 1 fF 0 g ½K fC i g K g fC i g ð16Þ while Eq. (5) becomes ) fPiþ1 g ¼ fPi g þ Dt k2 K g fC i g Ureolytic activity and calcium carbonate formation screening were conducted to determine the rate of urea hydrolysis and calcium carbonate precipitation respectively. 20 ml of tap water supplemented with 5.0 mM urea and 2.5 mM calcium was inoculated with a given bacterial cell concentration species 107 cell/ml in a flask. The test ran for 7 days with static incubation at 30 °C and pH 9 to simulate the real condition of concrete crack [39,40]. 0.5 ml of the solution was taken from the reaction flask every day to examine the evolution of urea and calcium carbonate concentration prior to centrifuging to remove the cells of bacteria and any suspended precipitation. For the examination of the former, the Nessler method was utilised to measure the ammonium concentration NH4+ in the solution via DR5000 UV-Vis Spectrophotometer at 425 nm [41]. As indicated earlier, NH4+ is produced by 1 mol of urea. Thus, the measured NH4+ could be converted to calculate the urea hydrolysis as expressed in Eq. (18). urea decomposed ðmg=LÞ ¼ Substituting Eq. (15) into Eq. (14), the Equation becomes 1 ffC iþ1 g Dt 3.1. Chemical analyses ð17Þ where P is Limestone precipitation 2.4. Procedure 1) Initialise the nodal variables with initial condition ct¼0 ¼ 0, external flux F 0 ¼ 0 and the concentration of urea on the left side of the crack is c = 333 mol/m3. 2) Solve system of Eqs. (16) and (17) at t = 1 3) Repeat the second step to obtain the C 2;3;4:::: and P2;3;4 for all other time steps until crack width fully filled with Limestone at S = 1. NH4ðmg=LÞ 60ðg=molÞ 2 18ðg=molÞ ð18Þ In the latter, the evolution of the microbial calcium carbonate was linked to the amount of insoluble calcium concentration to monitor the productivity rate. As such, the soluble calcium strength was first measured using an inductively coupled plasma atomic emission spectroscopy (Agilent 700 ICP-OES). Later, the insoluble calcium was calculated by subtracting the total calcium from the soluble calcium strength. A logistic curve fitting was used to obtain the rate of urea hydrolysis and calcium carbonate precipitation as shown in Eq. (19) [36]. y¼ a 1 þ ekðtbÞ ð19Þ where a is maximum capacity of y, it is time, b is the time at maximum y variation (dy/dx) and k is the rate constant (1/d) which was calculated from regression analysis. In addition, an experimental test was also conducted to confirm that the precipitation of the microbial calcium carbonate was 820 H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 dependent on the amount of urea hydrolysis in the proposed model. 50 ml of water supplemented with different urea concentration (5, 10, 15, 20, 30 g/L) was inoculated with bacteria in a flask. Calcium concentration was kept constant at 5 g/L, while yeast extract and peptone were added for bacterial growth. The solution was incubated under shaking (150 rpm) at 30 °C for 7 days. Subsequently, the calcium carbonate precipitation product was filtered through filter paper, which was then dried in the oven at 60 °C and weighed [42]. Finally, the smart lab x rays diffractometer (Rigoku) was used to analyse and identify the microbial product powder since XRD and 16 s rRNA sequence are considered as fingerprint techniques to identify solid material and bacteria strain, respectively. It was operated at 40 kV and 30 mA with Cu anode to produce intensive x rays spectra (CuKa radiation = 1.5418 Å), while, the diffracted patterns was collected using D/teX Ultra 250 detector over Bragg angle (2 theta3-100), 8.2551 deg/min, 0.0200 deg /step as continuous scans for 10 min. nied by nutrient (yeast extract 0.2%) for bacterial growth [43]. In addition, the bacterial cell concentration was kept at 107 cell/ml of mixing water prior to mortar mixing [44]. Next, 0.4 mm standard cracks were formed in the specimens after mixing by introducing a copper plate up to 20 mm deep, which was removed during the demolding of specimens [45]. Later, all specimens were cured in water and examined every two weeks to monitor the healing process. It is important to note that all specimens were assessed in triplicate. 3.2. Preparation of cracked specimens 4. Results and discussion Mortar specimens (U30, 50 mm) were casted using cement (OPC) Type I, tap water and river sand with 2.6 specific gravity according to BS EN 196-1:1995. The ratio of cement to sand was 1:3 by mass, while water cement ratio was 0.6. Urea and calcium nitrate were added into the mixing water to obtain 0.333 M urea and 0.15 M calcium for the urease enzyme activity and its function in bacterial aggregate formation respectively. This was accompa- 4.1. Nodal urea distribution 3.3. Vp-sem-edx VP-SEM-EDX (JEOL JSM-IT300LV Scanning Microscope) was utilised to verify the predicted crack-healing results [46]. Specifically, SEM was used to visualise the crack filling area every two weeks, while EDX analysis was conducted to better identify the filling product. When the capsule broke, urea was released into the water filled-crack, which was treated as big pore. The diffusion of urea through the pore path was not affected by any tortuosity or pore size in the proposed model since the targeted crack width was greater than 0.08 mm [47,48]. Consequently, the diffusion coeffi- Fig. 4. Discretised model for crack in concrete. Fig. 5. Nodal urea concentration in the crack domain without bacteria. H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 cient of urea was obtained from previous studies [49]. The amount of urea released into the crack domain from the crack’s left surface was maintained at a constant concentration and the other perimeter of the discretised model was assumed to be insulated to prevent any losses of urea outside the crack domain as shown in Fig. 4. Regardless of the size and shape of the capsule, only the amount of urea was taken into account in the present study’s model. Fig. 5 shows the concentration of urea in the crack at different times without bacteria. When there was no bacteria inside the crack domain, it began to increase without any hindrance until the equilibrium state was reached. As such, it could be said that the nodal concentration on all boundaries sought to go towards the boundary condition at node1. This state was known as the steady state, which was detected at t = 400 day. Moving on, Fig. 6 illustrates the nodal value of urea concentration in the cracks at different time with bacteria. According to Eqs. (4), and (9) the amount of urea that diffused from node 1 towards the rest of the boundary was depleted by the bacteria. The consumption by the bacteria induced the diffusive transport mechanism to the rest of the boundary. Thus, the urea consumption was proportional to the available concentration on the nodes. This mechanism continued until the equilibrium was achieved. The equilibrium state denoted that the amount of material that flows out is equal to the amount that is consumed. Fig. 6(c) shows that steady state conditions were attained at about t = 100 day. 4.2. Model convergence It should be demonstrated that the present study’s finite element model predicted a linear concentration distribution within each node as was indicated by the straight lines connecting the nodal urea concentration values. These nodal values were increased; that is, the number of elements was increased to ensure the accuracy and convergence of the solution as shown in Fig. 7. It should also be noted that the solution became smother when increasing the number of elements and four elements were taken into account since the difference was less than 1%. 821 Fig. 7. convergence of urea concentration using the numerical method. 4.3. Hydrolysis of urea Fig. 8(a) describes the dependence of the amount of urea hydrolysis on the concentration of urea, which is as expressed in Eq. (4). It shows that the amount of urea hydrolysis was significantly higher with 666 Mole/m3 urea compared to 333 Mole/m3. In addition, it was also observed that the amount of limestone was dependent on the amount of urea hydrolysis as show in Fig. 8(b). Owing to that, as urea hydrolysis increased, the amount of calcite (limestone) also increased. This predicted hypothesis was clearly confirmed through the authors’ experimental test, which was also consistent with the finding of previous studies [40]. Fig. 8(c) shows that the amount of calcite was linearly proportional to the amount of urea hydrolysis. With the increasing of urea concentration, more calcite could be formed. However, the mount of calcium and nutrient were kept at constant 5 g/L and 3 g/L respectively. Fig. 6. Nodal urea concentration with bacteria. 822 H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 Fig. 8. The dependence of Limestone on urea (a) Predicted urea hydrolysis (b) Predicted Limestone (c) Experimental data of produced Limestone with different concentration of urea (d) Identification of the product (Limestone) through XRD. Fig. 9. Comparison between actual and predicted crack healing ratio at 42 and 60 days (a and b) Predicted crack healing (b and c) Actual crack healing (e and f) Identification of the filling product (Limestone) using EDX. H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 In addition, The microbial product powder was recognised and identified as microbiological calcium carbonate precipitation by comparing the component of targeted sample to diffraction references data through XRD analysis since all solid material have a unique arrangement of atoms, similar to any living organism with unique DNA sequence. At 2h = 31°, the strongest reflection was achieved as shown in Fig. 8(d). 4.4. Calcite precipitation in the crack The present model observed the self-healing capacity of the artificial cracks in cementitous specimen. When the healing ratio (S) is equal to 1, it demonstrates that the crack volume is completely sealed with calcite, and thus the calculation stopped as shown in Equation 6. Fig. 9(a and b) illustrates the healing ratio in different times. Specifically, the 0.4 mm crack width was completely healed at 60 days, while predicted crack healing was 58% at time 42 days. In the same context, the laboratory data had a relatively high degree of similarity with the predicted results. This was obtained by monitoring the top surface of the cracked specimens every two weeks using VP-SEM images. It could be concluded that the 823 healing ratio increased with time and a crack width of 0.4 mm could be completely healed after 70 days, compared to 60 days in the model as shown in Fig. 9(c and d). The slight difference was due to two reasons. Firstly, the decreasing of porosity and interconnectivity of pores volume in the concrete with time due to cement hydration led to the difficulty of getting sufficient amount of oxygen, nutrient, nitrogen and calcium that is necessary for metabolic activity. Secondly, the viability of bacteria was affected by the increased age due to the continuing decreasing space, in which the bacteria occupied. Moreover, the crystal formation in the crack mouth was also identified as calcium carbonate due to the high peaks of Ca, O and C through EDX analysis. These ions were evident and their percentage was similar to the composition of calcium carbonate as shown in Fig. 9(e and f). At the same context, the verification of the proposed model was also made on the basis of the relationship between the predicted healing ratio and the actual filled area in the crack mouth. Both revealed relatively similar results with correlation coefficient (R = 0.99) as shown in Fig. 10. Correlation coefficient acted as a statistics indicator to show the strength of the results and fitting degree between the predicted output of the model and the experimental data. Fig. 10. Experimental test of crack healing compared with those predicted by proposed model (a) Predicted and actual crack healing ratio as function of time (b) Correlation of predicted and actual crack healing results. Fig. 11. healing ratio with different crack lengths at t = 42 days. 824 H.A. Algaifi et al. / Construction and Building Materials 189 (2018) 816–824 Furthermore, the effect of the crack length in x direction on selfhealing capacity was also observed. Fig. 11 shows that when the crack length decreased, the crack healing increased. 5. Conclusion The kinetics of calcite precipitation induced in response to the hydrolysis of urea by indigenous Lysinibacillus sphaericus in artificial concrete cracks were investigated. The amount of calcite depended on the amount of urea degradation, on the basis that the concentration of nutrient and calcium were sufficient for the bacterial activity. A mathematical model was developed based on a biochemical-diffusive concept. An ordinary differential equation and a second-order partial differential equation in time and space were numerically solved using finite element and finite difference method. The model was found to be applicable to highly reactive systems such as those proposed for engineering applications of MICP. Moreover, scanning electron microscopy (VP-SEM) with energy dispersive X-ray analysis (EDX) was used to verify the predicted crack healing results. Both showed a relative high degree of similarity with a correlation coefficient of R = 0.99. Conflict of interest None. Acknowledgements The authors acknowledge full gratitude to the Research University Grant (Tier 2 - Q.J130000.2622.15J43) for funding this research. This research activities were also supported and funded by the Ministry of Higher Education, Malaysia (MOHE) under the FRGS grant R.J130000.7822.4F722 and Universiti Teknologi Malaysia under the UTM COE research grant Q.J130000.2409.04G00. The authors would like to thank their support and cooperation in this research. 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